2022
DOI: 10.48550/arxiv.2212.04925
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Theoretical systematics in testing the Cosmological Principle with the kinematic quasar dipole

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Cited by 7 publications
(7 citation statements)
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“…A more recent study [133] succeeds in recovering the CMB dipole, but larger errors mean that the inferred dipole is consistent within 3σ with observations that claim an excess, such as, for example, [113] 33 . Separately, the Baldwin-Ellis methodology has been questioned [137][138][139]. These points aside, it is worth bearing in mind that these observations, along with [90,91], are serious claims that could potentially upend modern cosmology, but the results are preliminary.…”
Section: Prologuementioning
confidence: 99%
“…A more recent study [133] succeeds in recovering the CMB dipole, but larger errors mean that the inferred dipole is consistent within 3σ with observations that claim an excess, such as, for example, [113] 33 . Separately, the Baldwin-Ellis methodology has been questioned [137][138][139]. These points aside, it is worth bearing in mind that these observations, along with [90,91], are serious claims that could potentially upend modern cosmology, but the results are preliminary.…”
Section: Prologuementioning
confidence: 99%
“…Despite of the simplicity and overall observational consistency of the CP, a few challenges have developed during the past several years which appear to consistently question the validity of the CP on cosmological scales larger than 100M pc and motivate further tests to be imposed on its validity. Some of these challenges pointing to preferred directions on large cosmological scales include the quasar dipole [2][3][4][5][6], the radio galaxy dipole [7][8][9], the bulk velocity flow [10][11][12][13], the dark velocity flow [14], the CMB anomalies [15,16], the galaxy spin alignment [17][18][19], the galaxy cluster anisotropies [20], and a possible SnIa dipole [21,22]. These observational challenges of the CP may be indirectly connected with other tensions of the standard ΛCDM model including the Hubble [23][24][25] and growth ten- * leandros@uoi.gr sions [26][27][28][29] where the best fit parameter values of the model H 0 and σ 8 appear to be inconsistent when probed by different observational data.…”
Section: Introductionmentioning
confidence: 99%
“…In addition to the above theoretical challenges, the two main components in the ΛCDM model, dark matter (DM) and dark energy (DE), are poorly understood. Moreover, there are also some tensions between the cosmological and astrophysical observations and the ΛCDM model, which include the Hubble tension [3,[33][34][35][36][37][38][39][40] (5σ), growth tension [41][42][43] (2-3σ), CMB anisotropy anomalies [22,[44][45][46][47][48][49][50][51][52][53] (2-3σ), cosmic dipoles [23, [54][55][56][57][58][59][60][61][62][63] (2-5σ), Baryon Acoustic Oscillation (BAO) curiosities [64][65][66] (2.5-3σ), parity violating rotation of CMB linear polarization [67][68][69][70], small-scale curiosities [71][72][73][74], age of the universe [75], the Lithium problem [76] (2-4σ),the quasar Hu...…”
Section: Introductionmentioning
confidence: 99%